Physics, King's College London, The Strand, WC2R 2LS, London, UK.
Phys Chem Chem Phys. 2010 May 14;12(18):4759-67. doi: 10.1039/b920121a. Epub 2010 Mar 17.
The self-assembly of flat organic molecules on metal surfaces is controlled, apart from the kinetic factors, by the interplay between the molecule-molecule and molecule-surface interactions. These are typically calculated using standard density functional theory within the generalized gradient approximation, which significantly underestimates nonlocal correlations, i.e. van der Waals (vdW) contributions, and thus affects interactions between molecules and the metal surface in the junction. In this paper we address this question systematically for the Au(111) surface and a number of popular flat organic molecules which form directional hydrogen bonds with each other. This is done using the recently developed first-principles vdW-DF method which takes into account the nonlocal nature of electron correlation [M. Dion et al., Phys. Rev. Lett. 2004, 92, 246401]. We report here a systematic study of such systems involving completely self-consistent vdW-DF calculations with full geometry relaxation. We find that the hydrogen bonding between the molecules is only insignificantly affected by the vdW contribution, both in the gas phase and on the gold surface. However, the adsorption energies of these molecules on the surface increase dramatically as compared with the ordinary density functional (within the generalized gradient approximation, GGA) calculations, in agreement with available experimental data and previous calculations performed within approximate or semiempirical models, and this is entirely due to the vdW contribution which provides the main binding mechanism. We also stress the importance of self-consistency in calculating the binding energy by the vdW-DF method since the results of non-self-consistent calculations in some cases may be off by up to 20%. Our calculations still support the usually made assumption of the molecule-surface interaction changing little laterally suggesting that single molecules and their small clusters should be quite mobile at room temperature on the surface. These findings support a gas-phase modeling for some flat metal surfaces, such as Au(111), and flat molecules, at least as a first approximation.
除了动力学因素外,平面有机分子在金属表面上的自组装还受到分子间相互作用和分子与表面相互作用的控制。这些相互作用通常使用标准的密度泛函理论(在广义梯度近似下)进行计算,这会严重低估非局部相关性,即范德华(vdW)贡献,从而影响分子与结处金属表面之间的相互作用。在本文中,我们针对 Au(111)表面和一些常见的平面有机分子(它们彼此之间形成定向氢键)系统地研究了这个问题。这是通过最近开发的第一性原理 vdW-DF 方法完成的,该方法考虑了电子相关的非局域性质[M. Dion 等人,Phys. Rev. Lett. 2004, 92, 246401]。我们在这里报告了一个涉及完全自洽 vdW-DF 计算和全几何弛豫的此类系统的系统研究。我们发现,分子之间的氢键仅受到 vdW 贡献的轻微影响,无论是在气相中还是在金表面上。然而,与普通密度泛函(广义梯度近似,GGA)计算相比,这些分子在表面上的吸附能显著增加,这与可用的实验数据和先前在近似或半经验模型中进行的计算一致,而这完全是由于 vdW 贡献提供了主要的结合机制。我们还强调了 vdW-DF 方法计算结合能时自洽的重要性,因为在某些情况下,非自洽计算的结果可能会偏离多达 20%。我们的计算仍然支持通常的假设,即分子-表面相互作用在横向变化不大,这表明在室温下,单个分子及其小团簇在表面上应该具有相当的迁移能力。这些发现支持了在某些情况下对某些平面金属表面(如 Au(111))和平面分子进行气相建模,至少作为初步近似。